\begin{table}%t2
%\centering
\par
\caption{\label{table1.1}Physical properties of the cool H$_2$ component  from H$_2$ $v=0{-}0$ S(0)--S(2) lines extracted at the LL (10.5$\arcsec$) scale.}
\begin{tabular}{cccccc}
\hline \hline\noalign{\smallskip}%\\[-3.2mm]
Position & Offsets & H$_2$ 0--0 S(1)& $T$ & $N$(H$_2$)   & $\dot{M}$\tablefootmark{a} \\
		& (\arcsec) &	(10$^{-12}$ W~cm$^{-2}$ sr$^{-1}$)		& (K)  & 	(10$^{19}$~cm$^{-2}$) & (10$^{-6}~M_{\odot}$~yr$^{-1}$)\\
\hline
\par
R1+R2 & [--19.3, 15.1] & 1.4 &330 $\pm$ 50 & 7.5  & 2.0 \\
LL1 & [6.3, 2.0] & 1.3 &300 $\pm$ 45 & 7.8 &  2.8\\
\par
\hline
\end{tabular} 
\tablefoot{\tablefoottext{a}{$\dot{M}$ is proportional to ($V_{\rm jet}$/100~km~s$^{-1}$)~$\times$~(10.5$\arcsec$/$l_{\rm t}$) and is not
corrected for post-shock compression.}}
\vspace*{-3mm}
\end{table}